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illrrrrrrW

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The<br />

LOUJ-OhTn<br />

JJleter<br />

ALL RESISTORS :t~%<br />

Did you eyer try to get a good resistance<br />

read ing on a speaker voice coil?<br />

Or an automobile ignition balla st resistor? '<br />

Or a pilot light bu lb , length of coax, relay<br />

contact , loading coil, identi fy ing transformer<br />

windings, centertaps, etc .? If you<br />

have, then yo u' ve found that most ohmmet<br />

ers don' t have a rea lly low resista nc e<br />

scale - or if they do the zero set ting is<br />

unreliable and the meter scale inad equ at e.<br />

Aft er years of annoyan ce from this problem<br />

I finally decided that a low-value<br />

ohmmeter wou ld be a handy device to have<br />

around. In fact , applications for this meter<br />

just seem to suggest themselves. Why<br />

bother building a new version of an old<br />

instrument and not inc or porate new innovati<br />

ons? So I came up with the se requirements:<br />

• No zero ing knob - just a " set it<br />

and forget it" calibration cont rol.<br />

• Linear scale read ing from zero to a<br />

fixed value, rather than to inf inity.<br />

What good is infinity to an ohmmete<br />

r, besides making the upper<br />

25% or so of the scale relatively<br />

useless?<br />

• Solid terminal connectors rath er<br />

than wires with probes (optional).<br />

This would prevent poor contacts<br />

in the circui t, leading to error.<br />

The finished version uses one size D<br />

flashlight cell, has t wo scales - zero to<br />

lOQ, and zero to I Q . A " test" switch<br />

(momentary pushb utton) is used because<br />

of the high current requirem ent of the<br />

circuit. Battery life is conserved in this<br />

way.<br />

Theory of operation<br />

The circuit consists of a constant-<br />

FEBRUARY 1971<br />

A. Sch ecner W3YZ C<br />

122 She rry Lane Apts.<br />

Conshoho cken, PA 1942 8<br />

curr ent gen erator (Q 1) Lo provide a known<br />

Current through the test resistance. The<br />

voltage drop across this resistance (100 mV<br />

maximum) is read on a meter whose<br />

internal resistance is much higher than a<br />

test resistance of 10Q. Therefore , the<br />

met er does not load t he circuit.<br />

A bias for Ql is established by diodes<br />

Dl and D2 and resistors RI, R2 , R3, R4 ,<br />

and R5 . Use of the diod es hold s the bia s<br />

level constant desp ite nominal de cay of<br />

battery voltage. Diode D3 pr events severe<br />

overload of the meter in the absence of a<br />

test resistance. In case the test button is<br />

pres sed, the meter will overload, but not<br />

much, thanks to D3.<br />

My met er was "Obtained when I scrapped<br />

a Heath grid-dipper...... after bu ying a solidsta<br />

te model. The meter requiremen ts are<br />

500 IlA full scale, 200Q resista nce. A<br />

substitute may be constructed by using a<br />

mo re sensitive meter with a shun t, so long<br />

as the result is 500 IlA, 200n.<br />

Construction<br />

Layout is not critic al, but sold er connect<br />

ions must be solid and medium bus<br />

wire must be used. The battery connector<br />

mu st make tight connection with the batte<br />

ry . Check inte rn al resistance by shorting<br />

the test terminals wit h heavy wire. Pressing<br />

the test button should give a reading of<br />

zero.<br />

Transistor Q 1 may be replaced by any<br />

on e of a number of high-beta NPN typ es.<br />

Try .what yo u have around and see if it<br />

wor ks. R2 may be used to balan ce slight<br />

differences if another transistor is used.<br />

Calibrate by testing a precision IOn resi s­<br />

tor (O~10Q scale) and setting the calibration<br />

control for ,a full-scale reading. The<br />

other scale should foll ow automatic ally.<br />

87

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